Camera optical lens

ABSTRACT

The present disclosure relates to the field of optical lenses and provides a camera optical lens. The camera optical lens includes, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; a fourth lens having a positive refractive power; and a fifth lens having a negative refractive power. The camera optical lens satisfies following conditions: 0.80≤f1/f≤0.90; 70.00≤f3/f≤120.00; and −450.00≤(R5+R6)/(R5−R6)≤−430.00, where f denotes a focal length of the camera optical lens; f1 denotes a focal length of the first lens; f3 denotes a focal length of the third lens; R5 denotes a curvature radius of an object side surface of the third lens; and R6 denotes a curvature radius of an image side surface of the third lens.

TECHNICAL FIELD

The present disclosure relates to the field of optical lens, and more particularly, to a camera optical lens suitable for handheld terminal devices such as smart phones or digital cameras and camera devices such as monitors or PC lenses.

BACKGROUND

With the emergence of smart phones in recent years, the demand for miniature camera lens is increasing day by day, but in general the photosensitive devices of camera lens are nothing more than Charge Coupled Device (CCD) or Complementary Metal-Oxide Semiconductor Sensor (CMOS sensor), and as the progress of the semiconductor manufacturing technology makes the pixel size of the photosensitive devices become smaller, plus the current development trend of electronic products towards better functions and thinner and smaller dimensions, miniature camera lenses with good imaging quality therefore have become a mainstream in the market.

In order to obtain better imaging quality, the lens that is traditionally equipped in mobile phone cameras adopts a three-piece or four-piece lens structure. Also, with the development of technology and the increase of the diverse demands of users, and as the pixel area of photosensitive devices is becoming smaller and smaller and the requirement of the system on the imaging quality is improving constantly, a five-piece lens structure gradually appears in lens designs. Although the common five-piece lens has good optical performance, its settings on refractive power, lens spacing and lens shape still have some irrationality, which results in that the lens structure cannot achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

BRIEF DESCRIPTION OF DRAWINGS

Many aspects of the exemplary embodiment can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.

FIG. 1 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 1 of the present disclosure;

FIG. 2 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 1;

FIG. 3 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 1;

FIG. 4 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 1;

FIG. 5 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 2 of the present disclosure;

FIG. 6 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 5;

FIG. 7 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 5;

FIG. 8 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 5;

FIG. 9 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 3 of the present disclosure;

FIG. 10 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 9;

FIG. 11 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 9;

FIG. 12 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 9;

FIG. 13 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 4 of the present disclosure;

FIG. 14 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 13;

FIG. 15 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 13; and

FIG. 16 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 13.

DESCRIPTION OF EMBODIMENTS

The present disclosure will hereinafter be described in detail with reference to several exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of the present disclosure more apparent, the present disclosure is described in further detail together with the figure and the embodiments. It should be understood the specific embodiments described hereby is only to explain the disclosure, not intended to limit the disclosure.

Embodiment 1

Referring to FIG. 1, the present disclosure provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment 1 of the present disclosure. The camera optical lens 10 includes 5 lenses. Specifically, the camera optical lens 10 includes, from an object side to an image side, an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4 and a fifth lens L5. An optical element such as a glass plate GF can be arranged between the fifth lens L5 and an image plane Si. The glass plate GF can be a glass cover plate or an optical filter. In other embodiments, the glass plate GF can be arranged at other positions.

In present embodiment, the first lens L1 has a positive refractive power, and has an object side surface being a convex surface and an image object surface being a concave surface; the second lens L2 has a negative refractive power, and has an object side surface being a concave surface and an image object surface being a concave surface; the third lens L3 has a positive refractive power, and has an object side surface being a convex surface and an image object surface being a concave surface; the fourth lens L4 has a positive refractive power, and has an object side surface being a concave surface and an image object surface being a convex surface; and the fifth lens L5 has a negative refractive power, and has an object side surface being a convex surface and an image object surface being a concave surface.

Here, a focal length of the camera optical lens 10 is defined as f in a unit of millimeter (mm), a focal length of the first lens is defined as f1, a focal length of the third lens L3 is defined as f3, a curvature radius of the object side surface of the third lens is defined as R5, and a curvature radius of the image side surface of the third lens is defined as R6, where f, f1, f3, R5 and R6 should satisfy following conditions: 0.80≤f1/f≤0.90  (1); 70.00≤f3/f≤120.00  (2); and −450.00≤(R5+R6)/(R5−R6)≤−430.00  (3).

The condition (1) specifies a ratio of the focal length of the first lens L1 and the focal length of the camera optical lens 10. This leads to the appropriate distribution of the refractive power for the first lens L1, thereby facilitating correction of aberrations of the camera optical lens and thus improving the imaging quality.

The condition (2) specifies a ratio of the focal length of the third lens L3 and the focal length of the camera optical lens 10. This leads to the appropriate distribution of the refractive power for the third lens L3, thereby facilitating correction of aberrations of the camera optical lens and thus improving the imaging quality.

The condition (3) specifies a shape of the third lens L3. This can effectively correct aberrations generated by first two lenses (the first lens L1 and the second lens L2) in the camera optical lens.

In this embodiment, with the above configurations of the lenses including respective lenses having different refractive powers, in which there is a specific relationship between the focal length of the camera optical lens 10 and the first lens L1, there is a specific relationship between the focal length of the camera optical lens 10 and the third lens L3 and the third lens L3 has a specific shape, this leads to the appropriate distribution of the refractive power of the first lens L1 and the refractive power of the third lens L3, thereby facilitating correction of aberrations of the camera optical lens. This can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

In an example, a curvature radius of the object side surface of the first lens L1 is defined as R1 and a curvature radius of the image side surface of the first lens L1 is defined as R2, where R1 and R2 satisfy a condition of: −1.50≤(R1+R2)/(R1−R2)≤−1.35  (4).

The condition (4) specifies a shape of the first lens L1. Within this range, a development towards wide-angle lenses having a big aperture can alleviate a deflection degree of light passing through the lens, thereby effectively reducing aberrations.

In an example, a curvature radius of the object side surface of the second lens L2 is defined as R3, and R3 and f satisfy a condition of: −10.70≤R3/f≤−9.50  (5).

The condition (5) specifies a ratio of the curvature radius of the object side surface of the second lens L2 and the focal length of the camera optical lens 10. This can facilitate processing and assembly of the lenses.

In addition, a surface of a lens can be set as an aspherical surface. The aspherical surface can be easily formed into a shape other than the spherical surface, so that more control variables can be obtained to reduce the aberration, thereby reducing the number of lenses and thus effectively reducing a total length of the camera optical lens according to the present disclosure. In an embodiment of the present disclosure, both an object side surface and an image side surface of each lens are aspherical surfaces.

It should be noted that the first lens L1, the second lens L2, the third lens L3, the fourth lens L4 and the fifth lens L5 that constitute the camera optical lens 10 of the present embodiment have the structure and parameter relationships as described above, and therefore, the camera optical lens 10 can reasonably distribute the refractive power, the surface shape, the on-axis thickness and the like of each lens, and thus correct various aberrations. The camera optical lens 10 has Fno≤2.05. A total optical length from the object side surface of the first lens to an image plane of the camera optical lens along an optic axis (TTL) and an image height (IH) of the camera optical lens 10 satisfy a condition of TTL/IH≤1.50. The field of view (FOV) of the camera optical lens 10 satisfies FOV≥76.9 degrees. This can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

In an example, inflexion points and/or arrest points can be arranged on the object side surface and/or image side surface of the lens, so as to satisfy the demand for the high quality imaging. The description below can be referred to for specific implementations.

FIG. 1 is a schematic diagram of a structure of the camera optical lens 10 in accordance with Embodiment 1 of the present disclosure. The design information of the camera optical lens 10 in Embodiment 1 of the present disclosure is shown in the following. Table 1 lists curvature radiuses of object side surfaces and images side surfaces of the first lens L1 to the fifth lens L5 constituting the camera optical lens 10, central thicknesses of the lenses, distances between the lenses, the refractive index nd and the abbe number vd according to Embodiment 1 of the present disclosure. Table 2 shows conic coefficients k and aspheric surface coefficients. It should be noted that each of the distance, radii and the central thickness is in a unit of millimeter (mm).

TABLE 1 R d nd νd S1 ∞  d0= −0.284 R1 1.362  d1= 0.598 nd1 1.5439 ν1 55.95 R2 8.930  d2= 0.061 R3 −33.921  d3= 0.230 nd2 1.6614 ν2 20.41 R4 4.712  d4= 0.295 R5 5.969  d5= 0.245 nd3 1.6614 ν3 20.41 R6 5.996  d6= 0.425 R7 −9.224  d7= 0.742 nd4 1.5439 ν4 55.95 R8 −1.456  d8= 0.288 R9 2.724  d9= 0.350 nd5 1.5348 ν5 55.69 R10 0.869 d10= 0.407 R11 ∞ d11= 0.300 ndg 1.5168 νg 64.17 R12 ∞ d12= 0.398

In the table, meanings of various symbols will be described as follows.

R: curvature radius of an optical surface, a central curvature radius for a lens;

S1: aperture;

R1: curvature radius of the object side surface of the first lens L1;

R2: curvature radius of the image side surface of the first lens L1;

R3: curvature radius of the object side surface of the second lens L2;

R4: curvature radius of the image side surface of the second lens L2;

R5: curvature radius of the object side surface of the third lens L3;

R6: curvature radius of the image side surface of the third lens L3;

R7: curvature radius of the object side surface of the fourth lens L4;

R8: curvature radius of the image side surface of the fourth lens L4;

R9: curvature radius of the object side surface of the fifth lens L5;

R10: curvature radius of the image side surface of the fifth lens L5;

R11: curvature radius of an object side surface of the glass plate GF;

R12: curvature radius of an image side surface of the glass plate GF;

d: on-axis thickness of a lens or an on-axis distance between lenses;

d0: on-axis distance from the aperture S1 to the object side surface of the first lens L1;

d1: on-axis thickness of the first lens L1;

d2: on-axis distance from the image side surface of the first lens L1 to the object side surface of the second lens L2;

d3: on-axis thickness of the second lens L2;

d4: on-axis distance from the image side surface of the second lens L2 to the object side surface of the third lens L3;

d5: on-axis thickness of the third lens L3;

d6: on-axis distance from the image side surface of the third lens L3 to the object side surface of the fourth lens L4;

d7: on-axis thickness of the fourth lens L4;

d8: on-axis distance from the image side surface of the fourth lens L4 to the object side surface of the fifth lens L5;

d9: on-axis thickness of the fifth lens L5;

d10: on-axis distance from the image side surface of the fifth lens L5 to the object side surface of the optical filter GF;

d11: on-axis thickness of the glass plate GF;

d12: on-axis distance from the image side surface of the glass plate GF to the image plane Si;

nd: refractive index of d line;

nd1: refractive index of d line of the first lens L1;

nd2: refractive index of d line of the second lens L2;

nd3: refractive index of d line of the third lens L3;

nd4: refractive index of d line of the fourth lens L4;

nd5: refractive index of d line of the fifth lens L5;

ndg: refractive index of d line of the glass plate GF;

vd: abbe number;

v1: abbe number of the first lens L1;

v2: abbe number of the second lens L2;

v3: abbe number of the third lens L3;

v4: abbe number of the fourth lens L4;

v5: abbe number of the fifth lens L5;

vg: abbe number of the glass plate GF.

TABLE 2 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 A12 R1 −2.25273E+00   9.25156E−02   2.33465E−01 −1.87111E+00   8.58701E+00 −2.45136E+01 R2 −5.11829E+01 −1.03477E−01   1.52482E−01   2.99403E−01 −2.58332E+00   9.60967E+00 R3   2.59462E+02 −8.23886E−02   4.34597E−01 −3.00060E−01 −1.08449E+00   5.90051E+00 R4   1.16744E+01 −1.19745E−02   1.88221E−01   1.07954E+00 −7.71200E+00   2.72646E+01 R5 −8.35151E+01 −2.28897E−01   1.65661E−01 −1.76343E+00   8.76639E+00 −2.67375E+01 R6   8.99162E+00 −1.96981E−01 −4.55171E−03 −1.18108E−01   7.97616E−01 −2.44375E+00 R7   2.94505E+01   3.12669E−02 −2.02476E−01   3.86427E−01 −4.17330E−01   2.70476E−01 R8 −1.58546E+00 −4.86585E−02   7.06628E−02 −1.00258E−01   1.04016E−01 −2.03477E−02 R9 −6.45644E+01 −5.59339E−01   4.92446E−01 −2.76405E−01   1.24800E−01 −4.61134E−02  R10 −5.99645E+00 −2.45846E−01   2.05835E−01 −1.19021E−01   4.77649E−02 −1.33332E−02 Aspherical surface coefficients A14 A16 A18 A20 R1   4.38131E+01 −4.77942E+01 2.90409E+01 −7.55332E+00 R2 −2.30684E+01   3.33720E+01 −2.63903E+01   8.75582E+00 R3 −1.58468E+01   2.49571E+01 −2.12315E+01   7.51085E+00 R4 −5.90592E+01   7.92898E+01 −5.99823E+01   1.96735E+01 R5   4.96918E+01 −5.55761E+01   3.47874E+01 −9.34049E+00 R6   4.19597E+00 −4.14670E+00   2.28267E+00 −5.35694E−01 R7 −9.40240E−02   9.69382E−03   3.10908E−03 −6.98686E−04 R8 −2.66893E−02   1.75839E−02 −4.12933E−03   3.51165E−04 R9   1.30589E−02 −2.56794E−03   3.03901E−04 −1.60464E−05  R10   2.52931E−03 −3.12244E−04   2.28086E−05 −7.52477E−07

In Table 2, k is a conic coefficient, and A4, A6, A8, A10, A12, A14, A16, A18 and A20 are aspheric surface coefficients.

In the present embodiment, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above condition (6). However, the present disclosure is not limited to the aspherical polynomials form shown in the condition (6). Y=(x ² /R)/{1+[1−(1+k)(x ² /R ²)]^(1/2) }+A4x ⁴ +A6x ⁶ +A8x ⁸ +A10x ¹⁰ +A12x ¹² +A14x ¹⁴ +A16x ¹⁶ +A18x ¹⁸ +A20x ²⁰  (6)

Table 3 and Table 4 show design data of inflexion points and arrest points of respective lens in the camera optical lens 10 according to Embodiment 1 of the present disclosure. P1R1 and P1R2 represent the object side surface and the image side surface of the first lens L1, respectively, P2R1 and P2R2 represent the object side surface and the image side surface of the second lens L2, respectively, P3R1 and P3R2 represent the object side surface and the image side surface of the third lens L3, respectively, P4R1 and P4R2 represent the object side surface and the image side surface of the fourth lens L4, respectively, and P5R1 and P5R2 represent the object side surface and the image side surface of the fifth lens L5, respectively, respectively. The data in the column named “inflexion point position” refers to vertical distances from inflexion points arranged on each lens surface to the optic axis of the camera optical lens 10. The data in the column named “arrest point position” refers to vertical distances from arrest points arranged on each lens surface to the optic axis of the camera optical lens 10.

TABLE 3 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 1 0.865 P1R2 1 0.565 P2R1 1 0.345 P2R2 P3R1 1 0.235 P3R2 2 0.275 0.905 P4R1 1 1.385 P4R2 2 0.925 1.425 P5R1 3 0.205 1.135 1.835 P5R2 1 0.425

TABLE 4 Number of arrest points Arrest point position 1 P1R1 P1R2 1 0.745 P2R1 1 0.485 P2R2 P3R1 1 0.395 P3R2 1 0.465 P4R1 P4R2 P5R1 1 0.365 P5R2 1 1.145

In addition, Table 17 below further lists various values of Embodiment 1 and values corresponding to parameters which are specified in the above conditions.

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 435 nm, 486 nm, 546 nm, 587 nm and 656 nm after passing the camera optical lens 10 according to Embodiment 1. FIG. 4 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 10 according to Embodiment 1, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

In this embodiment, a full FOV of the camera optical lens is 2ω, and an F number is Fno, where 2ω=76.90° and Fno=2.04. Thus, the camera optical lens 10 can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

Embodiment 2

FIG. 5 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 2 of the present disclosure. Embodiment 2 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 5 and Table 6 show design data of a camera optical lens 20 in Embodiment 2 of the present disclosure.

TABLE 5 R d nd νd S1 ∞  d0= −0.271 R1 1.434  d1= 0.593 nd1 1.5439 ν1 55.95 R2 7.171  d2= 0.096 R3 −37.849  d3= 0.230 nd2 1.6614 ν2 20.41 R4 5.583  d4= 0.275 R5 5.199  d5= 0.245 nd3 1.6614 ν3 20.41 R6 5.223  d6= 0.454 R7 −13.448  d7= 0.617 nd4 1.5439 ν4 55.95 R8 −1.630  d8= 0.376 R9 1.977  d9= 0.344 nd5 1.5348 ν5 55.69 R10 0.809 d10= 0.407 R11 ∞ d11= 0.300 ndg 1.5168 νg 64.17 R12 ∞ d12= 0.403

TABLE 6 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 Al2 R1 −2.33918E+00   7.97661E−02   2.30798E−01 −1.85028E+00   8.55170E+00 −2.44722E+01 R2   2.01032E+01 −8.90670E−02   9.04449E−02   3.07323E−01 −2.54180E+00   9.64393E+00 R3 −2.26757E+01 −9.37952E−02   3.96302E−01 −2.97810E−01 −1.06611E+00   5.87510E+00 R4 −1.62740E+01 −4.58295E−02   1.90703E−01   1.13822E+00 −7.86692E+00   2.72290E+01 R5 −9.84283E+01 −2.39985E−01   1.62028E−01 −1.77458E+00   8.80340E+00 −2.67346E+01 R6 −1.56238E+01 −2.08600E−01   2.32248E−02 −1.44114E−01   8.03796E−01 −2.42600E+00 R7   1.00205E+01   3.77913E−02 −1.98760E−01   3.82567E−01 −4.15979E−01   2.70457E−01 R8 −1.00044E+00 −4.38909E−02   8.97865E−02 −1.05274E−01   1.03245E−01 −2.03202E−02 R9 −3.37736E+01 −5.69241E−01   4.87872E−01 −2.74245E−01   1.24905E−01 −4.61519E−02  R10 −5.81970E+00 −2.51830E−01   2.06960E−01 −1.18966E−01   4.77591E−02 −1.33346E−02 Aspherical surface coefficients A14 A16 A18 A20 R1   4.38065E+01 −4.77848E+01   2.90037E+01 −7.51825E+00 R2 −2.30620E+01   3.32837E+01 −2.65746E+01   9.04577E+00 R3 −1.58421E+01   2.48951E+01 −2.12737E+01   7.67863E+00 R4 −5.90565E+01   7.93562E+01 −5.99683E+01   1.94754E+01 R5   4.96531E+01 −5.56243E+01   3.48086E+01 −9.37684E+00 R6   4.20245E+00 −4.17456E+00   2.26099E+00 −5.03735E−01 R7 −9.41990E−02   9.64085E−03   3.11648E−03 −6.95268E−04 R8 −2.66367E−02   1.75994E−02 −4.12805E−03   3.50276E−04 R9   1.30489E−02 −2.56927E−03   3.04063E−04 −1.59464E−05  R10   2.52787E−03 −3.12023E−04   2.28553E−05 −7.59550E−07

Table 7 and Table 8 show design data of inflexion points and arrest points of respective lens in the camera optical lens 20 according to Embodiment 2 of the present disclosure.

TABLE 7 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 P1R2 1 0.585 P2R1 1 0.385 P2R2 P3R1 1 0.235 P3R2 2 0.275 0.905 P4R1 1 1.445 P4R2 2 0.895 1.415 P5R1 3 0.225 1.175 1.905 P5R2 1 0.415

TABLE 8 Number of arrest points Arrest point position 1 P1R1 P1R2 1 0.785 P2R1 1 0.555 P2R2 P3R1 1 0.395 P3R2 1 0.475 P4R1 P4R2 P5R1 1 0.415 P5R2 1 1.115

In addition, Table 17 below further lists various values of Embodiment 2 and values corresponding to parameters which are specified in the above conditions.

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 435 nm, 486 nm, 546 nm, 587 nm and 656 nm after passing the camera optical lens 20 according to Embodiment 2. FIG. 8 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 20 according to Embodiment 2, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

In the camera optical lens 20 according to this embodiment, 2ω=77.09° and Fno=2.02. Thus, the camera optical lens 20 can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

Embodiment 3

FIG. 9 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 3 of the present disclosure. Embodiment 3 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 9 and Table 10 show design data of a camera optical lens 30 in Embodiment 3 of the present disclosure.

TABLE 9 R d nd νd S1 ∞  d0= −0.271 R1 1.423  d1= 0.602 nd1 1.5439 ν1 55.95 R2 8.037  d2= 0.079 R3 −33.892  d3= 0.230 nd2 1.6614 ν2 20.41 R4 5.203  d4= 0.281 R5 5.083  d5= 0.245 nd3 1.6614 ν3 20.41 R6 5.106  d6= 0.458 R7 −12.954  d7= 0.622 nd4 1.5439 ν4 55.95 R8 −1.636  d8= 0.372 R9 2.153  d9= 0.346 nd5 1.5348 ν5 55.69 R10 0.843 d10= 0.407 R11 ∞ d11= 0.300 ndg 1.5168 νg 64.17 R12 ∞ d12= 0.398

TABLE 10 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 Al2 R1 −2.37278E+00   8.31528E−02   2.28202E−01 −1.86213E+00   8.57590E+00 −2.44922E+01 R2   5.19242E+00 −1.01352E−01   1.42605E−01   2.70534E−01 −2.55182E+00   9.64393E+00 R3   1.71438E+02 −9.06031E−02   4.35078E−01 −3.23773E−01 −1.07621E+00   5.87510E+00 R4 −3.63846E+00 −3.58796E−02   2.12104E−01   1.09003E+00 −7.81547E+00   2.72290E+01 R5 −7.29263E+01 −2.49061E−01   2.12080E−01 −1.85403E+00   8.85725E+00 −2.67346E+01 R6 −3.94406E+01 −1.86158E−01   2.22905E−02 −1.64168E−01   8.13780E−01 −2.41464E+00 R7   3.41814E+01   3.29994E−02 −1.94699E−01   3.80515E−01 −4.16008E−01   2.70581E−01 R8 −1.04590E+00 −4.76580E−02   8.86094E−02 −1.05080E−01   1.03355E−01 −2.03035E−02 R9 −3.66404E+01 −5.67257E−01   4.87268E−01 −2.74248E−01   1.24903E−01 −4.61516E−02  R10 −5.87868E+00 −2.51073E−01   2.06971E−01 −1.19079E−01   4.77764E−02 −1.33345E−02 Aspherical surface coefficients A14 A16 A18 A20 R1   4.38065E+01 −4.77848E+01   2.90037E+01 −7.51825E+00 R2 −2.30620E+01   3.32837E+01 −2.65746E+01   9.04577E+00 R3 −1.58421E+01   2.48951E+01 −2.12737E+01   7.67863E+00 R4 −5.90565E+01   7.93562E+01 −5.99683E+01   1.94754E+01 R5   4.96531E+01 −5.56243E+01   3.48086E+01 −9.37684E+00 R6   4.19283E+00 −4.17456E+00   2.26099E+00 −5.03735E−01 R7 −9.41551E−02   9.64716E−03   3.12057E−03 −6.99305E−04 R8 −2.66386E−02   1.75959E−02 −4.12925E−03   3.50582E−04 R9   1.30491E−02 −2.56917E−03   3.04072E−04 −1.59539E−05  R10   2.52766E−03 −3.12044E−04   2.28560E−05 −7.58648E−07

Table 11 and Table 12 show design data of inflexion points and arrest points of respective lens in the camera optical lens 30 according to Embodiment 3 of the present disclosure.

TABLE 11 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 0 P1R2 1 0.575 P2R1 1 0.365 P2R2 0 P3R1 1 0.245 P3R2 2 0.275 0.905 P4R1 0 P4R2 2 0.905 1.405 P5R1 3 0.225 1.175 1.895 P5R2 1 0.425

TABLE 12 Number of arrest points Arrest point position 1 P1R1 P1R2 1 0.755 P2R1 1 0.515 P2R2 P3R1 1 0.415 P3R2 1 0.475 P4R1 P4R2 P5R1 1 0.405 P5R2 1 1.115

In addition, Table 17 below further lists various values of Embodiment 3 and values corresponding to parameters which are specified in the above conditions.

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 435 nm, 486 nm, 546 nm, 587 nm and 656 nm after passing the camera optical lens 30 according to Embodiment 3. FIG. 12 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 30 according to Embodiment 3, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

In the camera optical lens 30 according to this embodiment, 2ω=76.89° and Fno=2.04. Thus, the camera optical lens 30 can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

Embodiment 4

FIG. 13 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 4 of the present disclosure. Embodiment 4 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 13 and Table 14 show design data of a camera optical lens 40 in Embodiment 2 of the present disclosure.

TABLE 13 R d nd νd S1 ∞  d0= −0.271 R1 1.389  d1= 0.589 nd1 1.5439 ν1 55.95 R2 8.130  d2= 0.069 R3 −33.862  d3= 0.230 nd2 1.6614 ν2 20.41 R4 5.095  d4= 0.290 R5 4.461  d5= 0.245 nd3 1.6614 ν3 20.41 R6 4.481  d6= 0.430 R7 −9.600  d7= 0.705 nd4 1.5439 ν4 55.95 R8 −1.534  d8= 0.329 R9 2.465  d9= 0.349 nd5 1.5348 ν5 55.69 R10 0.867 d10= 0.407 R11 ∞ d11= 0.300 ndg 1.5168 νg 64.17 R12 ∞ d12= 0.396

TABLE 14 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 A12 R1 −2.40108E+00   8.85574E−02   2.27518E−01 −1.87981E+00   8.58634E+00 −2.45154E+01 R2 −9.14171E+01 −1.24792E−01   1.67509E−01   2.98148E−01 −2.56736E+00   9.55383E+00 R3   4.56800E+02 −1.28374E−01   5.47221E−01 −3.71933E−01 −1.10286E+00   5.88407E+00 R4 −8.29098E+00 −3.23051E−02   2.94862E−01   1.01963E+00 −7.78714E+00   2.72946E+01 R5 −6.17086E+01 −2.36855E−01   2.04774E−01 −1.86084E+00   8.88411E+00 −2.67280E+01 R6 −2.02394E+01 −1.96070E−01   3.27250E−02 −1.63341E−01   8.05985E−01 −2.41623E+00 R7   4.08720E+01   2.80049E−02 −1.88535E−01   3.76277E−01 −4.14815E−01   2.70891E−01 R8 −1.57635E+00 −5.85958E−02   8.32983E−02 −1.04308E−01   1.03673E−01 −2.02432E−02 R9 −5.25328E+01 −5.54069E−01   4.83742E−01 −2.74180E−01   1.24903E−01 −4.61543E−02  R10 −6.04136E+00 −2.46094E−01   2.05440E−01 −1.19001E−01   4.77921E−02 −1.33331E−02 Aspherical surface coefficients A14 A16 A18 A20 R1   4.38153E+01 −4.77821E+01   2.89833E+01 −7.50386E+00 R2 −2.30901E+01   3.34811E+01 −2.62858E+01   8.59120E+00 R3 −1.57729E+01   2.50083E+01 −2.12146E+01   7.40231E+00 R4 −5.89829E+01   7.93057E+01 −6.00696E+01   1.96364E+01 R5   4.96246E+01 −5.56738E+01   3.48015E+01 −9.26334E+00 R6   4.19023E+00 −4.16823E+00   2.26433E+00 −5.12134E−01 R7 −9.42720E−02   9.52395E−03   3.11916E−03 −6.57935E−04 R8 −2.66387E−02   1.75869E−02 −4.13327E−03   3.51439E−04 R9   1.30508E−02 −2.56844E−03   3.04150E−04 −1.60084E−05  R10   2.52723E−03 −3.12101E−04   2.28569E−05 −7.57459E−07

Table 15 and Table 16 show design data of inflexion points and arrest points of respective lens in the camera optical lens 40 according to Embodiment 4 of the present disclosure.

TABLE 15 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 1 0.845 P1R2 1 0.335 P2R1 1 0.375 P2R2 P3R1 1 0.255 P3R2 2 0.295 0.915 P4R1 1 1.375 P4R2 2 0.925 1.405 P5R1 3 0.215 1.165 1.865 P5R2 1 0.425

TABLE 16 Number of arrest points Arrest point position 1 P1R1 P1R2 1 0.695 P2R1 1 0.515 P2R2 P3R1 1 0.435 P3R2 1 0.515 P4R1 P4R2 P5R1 1 0.385 P5R2 1 1.125

In addition, Table 17 below further lists various values of Embodiment 4 and values corresponding to parameters which are specified in the above conditions.

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 435 nm, 486 nm, 546 nm, 587 nm and 656 nm after passing the camera optical lens 40 according to Embodiment 4. FIG. 16 illustrates a field curvature and a distortion of light with a wavelength of 546 nm after passing the camera optical lens 40 according to Embodiment 4, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

In the camera optical lens 40 according to this embodiment, 2ω=76.90° and Fno=2.03. Thus, the camera optical lens 40 can achieve a high optical performance while satisfying design requirements for wide-angle and ultra-thin lenses having a big aperture.

Table 17 below lists various values of Embodiments 1, 2, 3 and 4 and values corresponding to parameters which are specified in the above conditions (1), (2), (3), (4) and (5) and values of relevant parameters.

TABLE 17 Embodi- Embodi- Embodi- Embodi- ment 1 ment 2 ment 3 ment 4 Notes f1/f 0.80 0.89 0.86 0.84 Condition (1) f3/f 118.99 93.88 89.93 70.98 Condition (2) (R5 + R6)/ −443.15 −434.25 −443.00 −447.10 Condition (R5 − R6) (3) (R1 + R2)/ −1.36 −1.50 −1.43 −1.41 Condition (R1 − R2) (4) R3/f −9.51 −10.70 −9.50 −9.51 Condition (5) Fno 2.04 2.02 2.04 2.03 2ω 76.90 77.09 76.89 76.9 f 3.567 3.538 3.567 3.561 f1 2.863 3.166 3.068 2.974 f2 −6.169 −7.256 −6.726 −6.604 f3 424.427 332.142 320.793 252.775 f4 3.062 3.334 3.363 3.242 f5 −2.541 −2.844 −2.844 −2.696 TTL 4.339 4.340 4.340 4.339 IH 2.911 2.911 2.911 2.911

It can be appreciated by one having ordinary skill in the art that the description above is only embodiments of the present disclosure. In practice, one having ordinary skill in the art can make various modifications to these embodiments in forms and details without departing from the spirit and scope of the present disclosure 

What is claimed is:
 1. A camera optical lens, comprising, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; a fourth lens having a positive refractive power; and a fifth lens having a negative refractive power, wherein the camera optical lens satisfies following conditions: 0.80≤f1/f≤0.90; 70.00≤f3/f≤120.00; and −450.00≤(R5+R6)/(R5−R6)≤−430.00, where f denotes a focal length of the camera optical lens; f1 denotes a focal length of the first lens; f3 denotes a focal length of the third lens; R5 denotes a curvature radius of an object side surface of the third lens; and R6 denotes a curvature radius of an image side surface of the third lens.
 2. The camera optical lens as described in claim 1, further satisfying a following condition: −1.50≤(R1+R2)/(R1−R2)≤−1.35, where R1 denotes a curvature radius of an object side surface of the first lens; and R2 denotes a curvature radius of an image side surface of the first lens.
 3. The camera optical lens as described in claim 1, further satisfying a following condition: −10.70≤R3/f≤−9.50, where R3 denotes a curvature radius of an object side surface of the second lens. 